NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = A.Basak Found 58 matches. 2023JO03 Nucl.Phys. A1031, 122610 (2023) F.Johora, D.Almalawi, M.Nure A.Abdullah, S.Hossain, Z.F.Shehadeh, A.K.Basak Non-monotonic potential description of α+209Bi elastic scattering NUCLEAR REACTIONS 209Bi(α, α), E=19-104 MeV; analyzed available data; deduced σ(θ), σ, potential parameters using the non-monotonic (NM) potential in the framework of optical model (OM).
doi: 10.1016/j.nuclphysa.2023.122610
2022BA24 Europhys.Lett. 138, 44002 (2022) A.K.Basak, A.C.Merchant, M.Freer, M.S.Islam, R.A.Ramon, M.Mizanur Rahman, A.S.B.Tariq, M.A.Uddin, A.Soylu 16O + 16O cluster states and their fusion to 32S: A non-monotonic potential description NUCLEAR REACTIONS 16O(16O, X)32S, E=25-1120 MeV; analyzed available data; calculated σ, rotational constants, potential families, quasi-molecular states, bands, optical and nuclear models potentials.
doi: 10.1209/0295-5075/ac6c48
2021IS08 J.Phys.(London) G48, 075109 (2021) M.S.Islam, R.A.Ramon, M.Mizanur Rahman, R.Majumder, M.A.Sayed, A.Nilima, M.M.B.Azad, A.S.B.Tariq, M.A.Uddin, A.K.Basak Nature of potential families from elastic 16O +16O rainbow scattering NUCLEAR REACTIONS 16O(16O, 16O), E=75-1120 MeV; analyzed available data; deduced optical potential parameters, σ.
doi: 10.1088/1361-6471/abd88e
2021IS12 J.Phys.(London) G48, 125108 (2021) M.S.Islam, R.A.Ramon, M.M.Rahman, M.S.Islam, M.M.B.Azad, A.S.B.Tariq, M.A.Uddin, S.Ali, A.K.Basak Primary rainbow and Airy minima in 12C + 12C elastic scattering with families of non-monotonic potentials NUCLEAR REACTIONS 12C(12C, 12C), E=25-360 MeV; analyzed available data; deduced σ, optical model parameters within the framework of the optical model (OM) using non-monotonic (NM) nucleus-nucleus potential.
doi: 10.1088/1361-6471/ac2fb0
2015HO06 Phys.Rev. C 91, 064613 (2015) S.Hossain, A.S.B.Tariq, A.Nilima, M.S.Islam, R.Majumder, M.A.Sayed, M.M.Billah, M.M.B.Azad, M.A.Uddin, I.Reichstein, F.B.Malik, A.K.Basak Dependence of the 16O+16O nuclear potential on nuclear incompressibility NUCLEAR REACTIONS 16O(16O, 16O), E=31.0, 41.0, 49.0, 59.0, 75.0, 80.6, 87.2, 92.4, 94.8, 98.6, 103.1, 115.9, 124.0, 145.0, 250.0, 350.0 MeV; analyzed σ(E, θ) data in the optical model using Nonmonotonic (NM) nucleus-nucleus potentials from energy-density functional (EDF) theory, and for nuclear incompressibility in K=188-266 MeV range.
doi: 10.1103/PhysRevC.91.064613
2015VI03 Pramana 85, 539 (2015) P.K.Vijayan, A.Basak, I.V.Dulera, K.K.Vaze, S.Basu, R.K.Sinha Conceptual design of Indian molten salt breeder reactor
doi: 10.1007/s12043-015-1070-0
2013HO02 Phys.Scr. 87, 015201 (2013) S.Hossain, M.N.A.Abdullah, Md.Zulfiker Rahman, A.K.Basak, F.B.Malik Non-monotonic potentials for 6Li elastic scattering at 88 MeV NUCLEAR REACTIONS 24,25,26Mg, 27Al, 40,44Ca, 59Co, 60Ni, 197Au, 206,208Pb(6Li, 6Li), E=88 MeV; analyzed available data, performance of the traditional phenomenological Woods-Saxon (WS) and squared WS potentials with that of a non-monotonic potential; deduced energy density functional, σ(θ). Comparison with available data.
doi: 10.1088/0031-8949/87/01/015201
2013HO16 J.Phys.(London) G40, 105109 (2013) S.Hossain, M.Billah, M.M.B.Azad, F.Parvin, M.N.A.Abdullah, K.M.Hasan, M.A.Uddin, A.S.B.Tariq, A.K.Basak, I.Reichstein, F.B.Malik Non-monotonic potential description of alpha-Zr refractive elastic scattering NUCLEAR REACTIONS 90Zr(α, α), E=15-141.7 MeV; analyzed available data; deduced scattering parameters, σ. Optical model framework using non-monotonic potentials.
doi: 10.1088/0954-3899/40/10/105109
2013UD01 Eur.Phys.J. D 67, 214 (2013) M.A.Uddin, A.K.F.Haque, T.I.Talukder, A.K.Basak, B.C.Saha, F.B.Malik Semi-empirical model for stopping cross sections of p, α and Li ions NUCLEAR REACTIONS Mo, Au(α, X), (p, X), (Li, X), E<100 MeV; calculated stopping σ for Z=2-100; Comparison with available data.
doi: 10.1140/epjd/e2013-40164-8
2011BA23 Europhys.Lett. 94, 62002 (2011) A.K.Basak, M.M.Billah, M.J.Kobra, M.K.Sarkar, M.Mizanur Rahman, Pretam K.Das, S.Hossain, M.N.A.Abdullah, A.S.B.Tariq, M.A.Uddin, S.Bhattacharjee, I.Reichstein, F.B.Malik Non-monotonic potentials and vector analyzing powers of 6, 7Li scattering by 12C, 26Mg, 58Ni, and 120Sn NUCLEAR REACTIONS 12C, 26Mg, 58Ni(6Li, 6Li), (7Li, 7Li), E=20 MeV; 120Sn(6Li, 6Li), (7Li, 7Li), E=44 MeV; calculated σ, vector analyzing power. Optical model potential, comparison with experimental data.
doi: 10.1209/0295-5075/94/62002
2009HO11 Eur.Phys.J. A 41, 215 (2009) S.Hossain, M.N.A.Abdullah, A.K.Basak, S.K.Das, M.A.Uddin, A.S.B.Tariq, I.Reichstein, K.M.Rusek, F.B.Malik Potential description of 6Li elastic scattering by 28Si NUCLEAR REACTIONS 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 22.8, 25.0, 27.0, 30.0, 34.0, 46.0, 75.6, 99.0, 135.0, 154.0, 210.0, 318.0 MeV; calculated σ(θ) using the energy-density functional formalism with different potentials; deduced parameters for the various potentials.
doi: 10.1140/epja/i2009-10813-7
2008HO15 Europhys.Lett. 84, 52001 (2008) S.Hossain, M.N.A.Abdullah, A.S.B.Tariq, M.A.Uddin, A.K.Basak, K.M.Rusek, I.Reichstein, F.B.Malik Microscopic 6Li-28Si potential from the energy-density functional theory NUCLEAR REACTIONS 28Si(7Li, 7Li), E=7.5-99.0 MeV; analyzed σ(θ).
doi: 10.1209/0295-5075/84/52001
2008TA01 Eur.Phys.J. D 46, 281 (2008) M.R.Talukder, S.Bose, M.A.R.Patoary, A.K.F.Haque, M.A.Uddin, A.K.Basak, M.Kando Empirical model for electron impact ionization cross sections of neutral atoms ATOMIC PHYSICS H, He, Li, C, N, O, F, Ne, Na, Mg, Al, Si, P, S, Cl, Ar, Fe, Cu, Ga, Ge, As, Se, Br, Kr, Ag, In, Sn, Sb, Te, I, Xe, Ba, Hg, Pb, Bi, U(e, X), E < 10 MeV; calculated electron impact total ionization cross sections for both open and closed shell neutral atoms using an empirical expression.
doi: 10.1140/epjd/e2007-00318-y
2006AB32 Nucl.Phys. A775, 1 (2006) M.N.A.Abdullah, M.S.Sabra, M.M.Rashid, Z.Shehadeh, M.M.Billah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Alpha-alpha potential up to 47.3 MeV bombarding energy NUCLEAR REACTIONS 4He(α, α), E=2.0-47.3 MeV; analysed σ, σ(θ); deduced parameters. 8Be deduced decay width. Various non-monotonic and Woods-Saxon α-nucleus potentials compared, phase shift effects discussed.
doi: 10.1016/j.nuclphysa.2006.06.007
2006HO04 Phys.Lett. B 636, 248 (2006) S.Hossain, M.N.A.Abdullah, K.M.Hasan, M.Asaduzzaman, M.A.R.Akanda, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, F.B.Malik Shallow folding potential for 16O + 12C elastic scattering NUCLEAR REACTIONS 16O(α, α), E=23.2-172.5 MeV; 12C(16O, 16O), E=132.0-260.0 MeV; calculated σ(θ). 12C deduced radius, α-cluster structure. Folding model, comparisons with data.
doi: 10.1016/j.physletb.2006.03.071
2005AB24 Nucl.Phys. A760, 40 (2005) M.N.A.Abdullah, A.B.Idris, A.S.B.Tariq, M.S.Islam, S.K.Das, M.A.Uddin, A.S.Mondal, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Potentials for the α- 40, 44, 48Ca elastic scattering NUCLEAR REACTIONS 40,44,48Ca(α, α), E=10-180 MeV; analyzed σ(θ); deduced parameters. Non-monotonic and Squared Woods-Saxon α-nucleus potentials compared, dispersion effects discussed.
doi: 10.1016/j.nuclphysa.2005.05.149
2005BI23 Nucl.Phys. A762, 50 (2005) M.M.Billah, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, I.Reichstein, H.M.Sen Gupta, F.B.Malik Alpha-Ni optical model potentials NUCLEAR REACTIONS 58,60,62,64Ni(α, α), E ≈ 15-166 MeV; calculated σ(θ). Four optical potentials compared with data.
doi: 10.1016/j.nuclphysa.2005.07.020
2005HO12 J.Phys.(London) G31, 309 (2005) S.Hossain, M.N.A.Abdullah, S.K.Das, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, I.J.Thompson, F.B.Malik Band mixing in 29Si and 29P NUCLEAR REACTIONS 28Si(α, t), (α, 3He), E=45 MeV; analyzed σ(E, θ). 29P, 29Si deduced configurations, band-mixing effects. Coupled channels approach, finite-range transfer theory, Nilsson model.
doi: 10.1088/0954-3899/31/5/003
2003AB11 J.Phys.(London) G29, 1259 (2003) M.N.A.Abdullah, S.K.Das, A.S.B.Tariq, M.S.Mahbub, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Molecular versus squared Woods-Saxon α-nucleus potentials in the 27Al(α, t)28Si reaction NUCLEAR REACTIONS 27Al(α, t), (α, α), E=64.5 MeV; calculated σ(θ), σ(E, θ). Comparison of Woods-Saxon and molecular potentials, comparison with data.
doi: 10.1088/0954-3899/29/6/323
2003AB22 Phys.Lett. B 571, 45 (2003) M.N.A.Abdullah, M.S.I.Sarker, S.Hossain, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik Cluster structure of 40, 44, 48Ca NUCLEAR REACTIONS 40,44,48Ca(α, α), E=22-166 MeV; analyzed σ(θ); deduced parameters. 40,44,48Ca deduced α-cluster structure. Folded potential.
doi: 10.1016/j.physletb.2003.08.014
2003AB24 Eur.Phys.J. A 18, 65 (2003) M.N.A.Abdullah, S.Hossain, M.S.I.Sarker, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, S.Ali, H.M.Sen Gupta, F.B.Malik Cluster structure of 16O NUCLEAR REACTIONS 16O(α, α), E=25.4-146.0 MeV; calculated σ(θ). 16O deduced radius. Folding model, α-cluster configurations, comparisons with data.
doi: 10.1140/epja/i2003-10068-7
2002AB22 Eur.Phys.J. A 15, 477 (2002) M.N.A.Abdullah, M.S.Mahbub, S.K.Das, A.S.B.Tariq, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Investigation of α-nucleus interaction in the 27Al(α, α)27Al scattering and 27Al(α, d)29Si reaction NUCLEAR REACTIONS 27Al(α, α), E=22.3-64.5 MeV; analyzed σ(θ); deduced potential parameters. 27Al(α, d), E=26.5, 27.2 MeV; calculated spectroscopic factors, σ(θ). Molecular and Michel potentials, DWBA.
doi: 10.1140/epja/i2002-10066-0
2001BB08 Eur.Phys.J. A 12, 387 (2001) A.K.Basak, M.N.A.Abdullah, A.S.B.Tariq, S.K.Das, A.F.M.M.Rahman, A.S.Mondal, H.M.Sen Gupta, F.B.Malik Investigation of Inelastic α-Scattering on 24Mg and 28Si NUCLEAR REACTIONS 24Mg(α, α'), E=54 MeV; 28Si(α, α'), E=26 MeV; measured σ(E, θ); deduced potential parameters. Coupled channels analysis.
doi: 10.1007/s10050-001-8662-4
2001DA19 Phys.Rev. C64, 034605 (2001) S.K.Das, A.S.B.Tariq, A.F.M.M.Rahman, S.Hossain, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik Effect of the α-Nucleus Interaction on the 29, 30Si(α, d)31, 32P Reaction NUCLEAR REACTIONS 29,30Si(α, d), E=25 MeV; calculated σ(E, θ), spectroscopic factors. Microscopic and macroscopic DWBA calculations, comparison of molecular, standard and squared Woods-Saxon α-nucleus potentials.
doi: 10.1103/PhysRevC.64.034605
2000DA28 Phys.Rev. C62, 054605 (2000) S.K.Das, A.S.B.Tariq, M.A.Uddin, A.S.Mondal, A.K.Basak, K.M.Rashid, H.M.Sen Gupta, F.B.Malik Effect of α-Nucleus Potential on the 28Si(α, d)30P Reaction NUCLEAR REACTIONS 28Si(α, d), E=26 MeV; analyzed σ(E, θ). 30P level deduced J, π. DWBA calculations, several potentials compared.
doi: 10.1103/PhysRevC.62.054605
2000DA29 Phys.Rev. C62, 054606 (2000) S.K.Das, A.K.Basak, K.Banu, A.S.Mondal, A.S.B.Tariq, A.F.M.M.Rahman, H.M.Sen Gupta, F.B.Malik Effect of the α-Nucleus Potential on the 28Si(α, p)31P Reaction NUCLEAR REACTIONS 28Si(α, α), (α, p), E=26 MeV; analyzed σ(E, θ). DWBA calculations, several potentials compared.
doi: 10.1103/PhysRevC.62.054606
1999DA20 Phys.Rev. C60, 044617 (1999); Comment Phys.Rev. C62, 049801 (2000) S.K.Das, A.S.B.Tariq, A.F.M.Rahman, R.K.Roy, M.N.Huda, A.S.Mondal, A.K.Basak, H.M.Sen Gupta, F.B.Malik Effect of α-Nucleus Potential on the 27Al(α, t)28Si Reaction NUCLEAR REACTIONS 27Al(α, α), E=64.5 MeV; analyzed σ(θ); deduced parameters. 27Al(α, t), E=64.5 MeV; calculated σ(E, θ). 28Si deduced spectroscopic factors. Finite-range DWBA, molecular and Michel optical potentials. Comparisons with data.
doi: 10.1103/PhysRevC.60.044617
1999DA24 Nuovo Cim. 112A, 661 (1999) S.K.Das, A.K.Basak, A.S.Mondal, A.S.B.Tariq, A.F.M.Rahman, D.R.Sarker, H.M.Sen Gupta Normalization Constant of the (α, t) Reaction NUCLEAR REACTIONS 16O, 19F, 25Mg, 27Al, 30Si, 40Ca, 51V, 55Mn, 54Fe, 59Co, 64Ni, 116Sn, 144Sm, 208Pb(α, t), E=25-104 MeV; analyzed σ(θ); deduced normalization constant. DWBA analysis.
doi: 10.1007/BF03035876
1999TA13 Phys.Rev. C59, 2558 (1999) A.S.B.Tariq, A.F.M.M.Rahman, S.K.Das, A.S.Mondal, M.A.Uddin, A.K.Basak, H.M.Sen Gupta, F.B.Malik Potential Description of Anomalous Large Angle Scattering of α Particles NUCLEAR REACTIONS 28Si(α, α), E=14.47-45 MeV; 30Si(α, α), E=26.6 MeV; 24Mg(α, α), E=22-120 MeV; analyzed σ(θ); deduced potential parameters. Michel, molecular potentials, anomalous large angle scattering.
doi: 10.1103/PhysRevC.59.2558
1998HA68 Nuovo Cim. 111, 1131 (1998) M.Haque, S.K.Das, A.K.Basak, H.M.Sen Gupta Anomaly in the Normalization Constant of the (3He, p) Reaction NUCLEAR REACTIONS 62Ni(3He, p), E not given; calculated DWBA normalization constants; deduced dependence on final level, possible multi-step mechanisms.
1997BA60 Phys.Rev. C56, 1983 (1997) A.K.Basak, M.A.Basher, A.S.Mondal, M.A.Uddin, S.Bhattacherjee, A.Husain, S.K.Das, M.Haque, H.M.Sen Gupta 64Cu Levels from the 62Ni(3He, p) Reaction at 18 MeV NUCLEAR REACTIONS 62Ni(3He, p), E=18 MeV; measured proton spectra, σ(Ep, θ); deduced optical model parameters. 64Cu levels deduced J, π. Shell model analysis.
doi: 10.1103/PhysRevC.56.1983
1992BA16 Phys.Rev. C45, 1575 (1992) M.A.Basher, H.R.Siddique, A.Husain, A.K.Basak, H.M.Sen Gupta Level Structure of 52Cr from the 51V(3He, d) Reaction NUCLEAR REACTIONS 51V(3He, d), E=15 MeV; measured σ(θ). 52Cr deduced levels, L, J, π, spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.45.1575
1989BA24 Nucl.Phys. A499, 353 (1989) Parity-Violating Effects in the 6Li(α, γ)10B Capture Reaction via the 5.1 MeV Doublet Resonance NUCLEAR REACTIONS 6Li(α, γ), E=1.085, 1.175 MeV; measured σ(θ). 10B levels deduced γ-transition strengths, mixing ratio. Enriched target.
doi: 10.1016/0375-9474(89)90051-1
1987WA21 Nucl.Phys. A470, 339 (1987) R.E.Warner, B.A.Vaughan, J.A.Ditusa, J.W.Rovine, R.S.Wakeland, C.P.Browne, S.E.Darden, S.Sen, A.Nadasen, A.Basak, T.R.Donoghue, T.Rinckel, K.Sale, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster The Mechanism of the 7Li(d, 2α)n Reaction from E(d) = 3 to 15 MeV NUCLEAR REACTIONS, MECPD 7Li(d, 2α), E=3-15 MeV; measured σ(θ1, θ2) vs energy difference; deduced reaction mechanism. 8Be deduced levels. Enriched 7LiF targets.
doi: 10.1016/0375-9474(87)90006-6
1986DR03 Nucl.Phys. A448, 93 (1986) P.V.Drumm, O.Karban, A.K.Basak, P.M.Lewis, S.Roman, G.C.Morrison Study of 14N by One-Nucleon Transfer Reactions Induced with Polarised 3He NUCLEAR REACTIONS 13C, 15N(polarized 3He, 3He), 13C(polarized 3He, d), 15N(polarized 3He, α), E=33 MeV; measured σ(θ), A(θ); deduced optical-model parameters. 14N levels deduced j-transfer values, S(lj).
doi: 10.1016/0375-9474(86)90182-X
1984TO12 Phys.Lett. 149B, 9 (1984) J.A.Tostevin, J.M.Nelson, O.Karban, A.K.Basak, S.Roman Direct Observation of the Alpha Particle D-State in the (d, α) Reaction NUCLEAR REACTIONS 40Ca(polarized d, α), E=12.3 MeV; calculated σ(θ), vector analyzing power vs θ; deduced α-particle D-state role. DWBA, cluster transfer.
doi: 10.1016/0370-2693(84)91540-5
1983LE03 Nucl.Phys. A395, 204 (1983) P.M.Lewis, A.K.Basak, J.D.Brown, P.V.Drumm, O.Karban, E.C.Pollacco, S.Roman The Elastic and Inelastic Scattering of 33 MeV Polarized 3He from Oxygen and Iron Isotopes NUCLEAR REACTIONS 17,18O, 54,56Fe(polarized 3He, 3He), (polarized 3He, 3He'), E=33 MeV; measured σ(θ), A(θ); deduced optical model parameters, deformation parameters. Enriched targets.
doi: 10.1016/0375-9474(83)90096-9
1982KA12 Phys.Lett. 112B, 433 (1982) O.Karban, A.K.Basak, P.M.Lewis, S.Roman Configurations of Particle-Hole States in 16O NUCLEAR REACTIONS 17O(polarized 3He, α), E=33 MeV; measured σ(θ), analyzing power vs θ. 16O levels deduced L, j-transfer, C2S, configurations. DWBA analysis.
doi: 10.1016/0370-2693(82)90842-5
1981BA37 Nucl.Phys. A368, 74 (1981) A.K.Basak, O.Karban, S.Roman, G.C.Morrison, C.O.Blyth, J.M.Nelson Scattering and Charge-Exchange Reactions with Polarized 3He on Lithium Isotopes NUCLEAR REACTIONS 6,7Li(polarized 3He, 3He), (polarized 3He, 3He'), (polarized 3He, t), E=33.3 MeV; measured σ(θ), A(θ); deduced optical-model parameters, reaction mechanism. Enriched 6Li target.
doi: 10.1016/0375-9474(81)90731-4
1981BA38 Nucl.Phys. A368, 93 (1981) A.K.Basak, O.Karban, S.Roman, G.C.Morrison, C.O.Blyth, J.M.Nelson Polarization Effects in 3He Induced Transfer Reactions on Lithium Isotopes NUCLEAR REACTIONS 6,7Li(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ). 7,8Be, 5,6Li levels deduced S. Enriched 6Li target. DWBA, coupled-channels analyses.
doi: 10.1016/0375-9474(81)90732-6
1981EN04 Nucl.Phys. A366, 1 (1981) F.Entezami, A.K.Basak, O.Karban, P.M.Lewis, S.Roman Interactions of Polarized 3He Particles with 24Mg NUCLEAR REACTIONS 24Mg(polarized 3He, 3He), (polarized 3He, 3He'), (polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ); deduced contribution of two-step processes. Enriched target. DWBA, coupled-channels analysis.
doi: 10.1016/0375-9474(81)90483-8
1981KA24 Nucl.Phys. A366, 68 (1981) O.Karban, A.K.Basak, F.Entezami, S.Roman Spectroscopy of 62Ni with the 61Ni(d(pol), p) Reaction NUCLEAR REACTIONS 61Ni(polarized d, p), E=12.3 MeV; measured σ(θ), iT11, T20, T22 vs (θ). 62Ni deduced levels, L, j-transfer, π, (2J+1)S. Enriched target.
doi: 10.1016/0375-9474(81)90488-7
1981KA38 Nucl.Phys. A369, 38 (1981) O.Karban, A.K.Basak, F.Entezami, P.M.Lewis, S.Roman Analysing Powers of the 54Fe(3He(pol), d)55Co and 54Fe(3He(pol), α)53Fe Reactions NUCLEAR REACTIONS 54Fe(polarized 3He, d), (polarized 3He, α), E=33 MeV; measured σ(θ), A(θ). 55Co, 53Fe levels deduced J, π, C2S, j-dependence. Enriched target.
doi: 10.1016/0375-9474(81)90005-1
1980OK04 Nucl.Phys. A349, 339 (1980) N.T.Okumusoglu, A.K.Basak, C.O.Blyth Analyzing Powers in the Three-Body Break-Up Reactions from 3He(pol) + 2H NUCLEAR REACTIONS 2H(polarized 3He, 2p), (polarized 3He, pt), (polarized 3He, p3He), E=33 MeV; measured σ(Ep, θ1, θ2), analyzing power vs Ep.
doi: 10.1016/0375-9474(80)90291-2
1978BA13 Nucl.Phys. A295, 111 (1978) A.K.Basak, J.A.R.Griffith, O.Karban, J.M.Nelson, S.Roman Tensor Analysing Powers of (d, p) Reactions on 28Si, 67Zn, 90Zr and 208Pb at 12.3 MeV NUCLEAR REACTIONS 28Si, 67Zn, 90Zr, 208Pb(polarized d, p), E=12.3 MeV; measured analyzing powers iT11(θ), T20(θ); deduced J-transfers. 68Zn level deduced J, π. Natural 28Si; enriched 67Zn, 90Zr, 208Pb targets.
doi: 10.1016/0375-9474(78)90023-4
1978LU05 Nucl.Phys. A297, 189 (1978) Y.-W.Lui, O.Karban, A.K.Basak, C.O.Blyth, J.M.Nelson, S.Roman Scattering of Polarized 3He by 4He between 18 and 32 MeV NUCLEAR REACTIONS 4He(polarized 3He, 3He), E=18-32 MeV; measured A(θ); deduced phase shifts. 7Be deduced level, J, π.
doi: 10.1016/0375-9474(78)90271-3
1978TU07 Fizika, Suppl. 10, 51 (1978) G.Tungate, J.A.R.Griffith, O.Karban, A.K.Basak Elastic Scattering of 12.4 MeV Tensor Polarized Deuterons NUCLEAR REACTIONS 64Ni, 65Cu, 90Zr(polarized d, d), E=12.4 MeV; measured σ(θ), iT11(θ), T20(θ), T22(θ). Optical model analysis with tensor terms.
1977BA04 Nucl.Phys. A275, 381 (1977) A.K.Basak, J.A.R.Griffith, O.Karban, J.M.Nelson, S.Roman, G.Tungate Polarization Transfer in the 28Si(d, p)29Si(g.s.) Reaction and Deuteron D-State Effects NUCLEAR REACTIONS 28Si(polarized d, p), E=12.1 MeV; measured polarization transfer coefficient at θ(lab)=10°, 20°; deduced evidence of deuteron d-state contribution.
doi: 10.1016/0375-9474(77)90459-6
1977BA14 Nucl.Phys. A278, 217 (1977) A.K.Basak, J.A.R.Griffith, M.Irshad, O.Karban, E.J.Ludwig, J.M.Nelson, S.Roman, G.Tungate Spectroscopy of the 50Cr(d, p)51Cr Reaction and the Deuteron d-State Effects NUCLEAR REACTIONS 50Cr(polarized d, p), E=12.3 MeV; measured analyzing powers iT11(θ), T20(θ), T22(θ). 51Cr levels deduced J. Enriched target.
doi: 10.1016/0375-9474(77)90236-6
1977BA39 Nucl.Phys. A286, 420 (1977) A.K.Basak, J.A.R.Griffith, O.Karban, S.Roman, G.Tungate Analysing Powers of the (d, p) and (d, t) Reactions Induced by 12 MeV Polarized Deuterons in the 1p Shell NUCLEAR REACTIONS 9Be(polarized d, p), 9Be(polarized d, t), E=12 MeV; measured iT11, T20, T22(θ); 12C(polarized d, p), E=12.3 MeV; measured T20, T22; deduced J-mixing ratio. Natural targets.
doi: 10.1016/0375-9474(77)90593-0
1977KA10 J.Phys.(London) G3, 571 (1977) O.Karban, A.K.Basak, C.O.Blyth, W.Dahme, J.B.A.England, J.M.Nelson, N.T.Okumusoglu, S.Roman, G.G.Shute, R.Vlastou Scattering of 33 MeV Polarized 3He Particles by Hydrogen and Helium Isotopes NUCLEAR REACTIONS 1,2,3H, 3,4He(polarized 3He, 3He), E=33.3 MeV; measured A(θ); deduced optical-model parameters.
doi: 10.1088/0305-4616/3/4/017
1977RO12 Nucl.Phys. A284, 365 (1977) S.Roman, A.K.Basak, J.B.A.England, O.Karban, G.C.Morrison, J.M.Nelson Polarization Effects in the Elastic Scattering of 3He and (3He, d) Reaction on 58Ni NUCLEAR REACTIONS 58Ni(polarized 3He, 3He), 58Ni(polarized 3He, d), E=33.3 MeV; measured A(θ). Enriched target.
doi: 10.1016/0375-9474(77)90390-6
1977RO17 Nucl.Phys. A289, 269 (1977) S.Roman, A.K.Basak, J.B.A.England, J.M.Nelson, N.E.Sanderson, F.D.Santos, A.M.Eiro 3He D-State Effects in (d, 3He) Reactions NUCLEAR REACTIONS 27Al(polarized d, 3He), E=12.4 MeV; measured iT11, T20, T22(θ); deduced 3He d-state contribution. Natural target.
doi: 10.1016/0375-9474(77)90032-X
1976KA20 Nucl.Phys. A266, 413 (1976) O.Karban, A.K.Basak, J.A.R.Griffith, S.Roman, G.Tungate Tensor Analysing Powers in Deuteron Elastic Scattering by 50Cr, 66Zn and 67Zn NUCLEAR REACTIONS 50Cr, 66,67Zn(d, d), E=12.4 MeV; measured σ(θ), iT11, T20, T22(θ); deduced tensor optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(76)90367-5
1976KA23 Nucl.Phys. A269, 312 (1976) O.Karban, A.K.Basak, J.B.A.England, G.C.Morrison, J.M.Nelson, S.Roman, G.G.Shute The j-Dependence of (3He, d) and (3He, α) Reaction Analysing Powers in the 1p Shell NUCLEAR REACTIONS 9Be, 12C(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ); deduced J-dependence. 10B, 8Be, 13N, 11C levels deduced S.
doi: 10.1016/0375-9474(76)90683-7
1976SA26 Phys.Rev.Lett. 37, 1672 (1976) N.E.Sanderson, A.K.Basak, J.B.A.England, J.M.Nelson, S.Roman Investigation of d5/2-d3/2 Admixing in the Pickup Strength to the First Excited States of 22Ne and 26Mg NUCLEAR REACTIONS 23Na, 27Al(polarized d, 3He), E=12.4 MeV; measured vector analyzing power iT11; deduced admixing in pickup strength to levels in 22Ne, 26Mg.
doi: 10.1103/PhysRevLett.37.1672
1974BA49 Nucl.Phys. A229, 219 (1974) A.K.Basak, J.A.R.Griffith, M.Irshad, O.Karban, E.J.Ludwig, J.M.Nelson, S.Roman Vector Analyzing Power of (d, p) and (d, t) Reactions on 142Nd at 12.3 MeV NUCLEAR REACTIONS 142Nd(polarized d, d), (polarized d, p), (polarized d, t), E=12.3 MeV; measured iT11(θ); deduced optical-model parameters, reaction characteristics. 143Nd levels deduced L(n), J, S; 141Nd levels deduced L(n), J. Enriched target.
doi: 10.1016/0375-9474(74)90784-2
1971HU18 Nucleus (Lahore) 8, 55 (1971) A.Husain, M.M.Kasim, A.K.Basak, A.S.Mandal, P.Ali, B.C.Saha The Lifetime of Heavy Spallation Hyperfragments
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